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Page 298
... side . But far away from the hole ( in terms of its dimensions ) , although still " near the conducting plane ... side of the perfectly conducting sheet which is an equipotential surface . Similarly for the magnetic induction , B must be ...
... side . But far away from the hole ( in terms of its dimensions ) , although still " near the conducting plane ... side of the perfectly conducting sheet which is an equipotential surface . Similarly for the magnetic induction , B must be ...
Page 555
... sides with a typical Xim , and integrate over all angles . All the terms on the left - hand side of the equation involving gim ( r ) vanish because of orthogonality , and only one term involving an fim ( r ) survives : ď2 2 d + + k2 ...
... sides with a typical Xim , and integrate over all angles . All the terms on the left - hand side of the equation involving gim ( r ) vanish because of orthogonality , and only one term involving an fim ( r ) survives : ď2 2 d + + k2 ...
Page 567
... sides of ( 16.22 ) . Then we can put | x − x ' ~ r ' n.x on the left - hand side , where n is a unit vector in the direction of x ' . On the right side r > r ' and r = r . Furthermore we can - = < use the asymptotic form ( 16.13 ) for ...
... sides of ( 16.22 ) . Then we can put | x − x ' ~ r ' n.x on the left - hand side , where n is a unit vector in the direction of x ' . On the right side r > r ' and r = r . Furthermore we can - = < use the asymptotic form ( 16.13 ) for ...
Contents
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ